Response of stomatal conductance, transpiration, and photosynthesis to light and CO2 for rice leaves with different appearance days

To investigate the dynamics of stomata, transpiration, and photosynthesis under varying light intensities and CO2 conditions during leaf development, the light response and CO2 response of stomatal conductance (g sw), transpiration rate (T r), and net photosynthetic rate (P n) were observed for rice leaves at different days after leaf emergence (DAE). The results showed that (1) as photosynthetically active radiation (PAR) increased, leaf g sw, T r, and P n initially increased rapidly and linearly, followed by a more gradual rise to maximum values, and then either stabilized or showed a declining trend. The maximum g sw, T r, and P n were smaller and occurred earlier for old leaves than for young leaves. The g sw, T r, and P n all exhibited a linear decreasing trend with increasing DAE, and the rate of decrease slowed down with the reduction in PAR; (2) as the CO2 concentration (C a) increased, g sw and T r decreased gradually to a stable minimum value, while P n increased linearly and slowly up to the maximum and then kept stable or decreased. The g sw, T r, and P n values initially kept high and then decreased with the increase of DAE. These results contribute to understanding the dynamics in g sw, T r, and P n during rice leaf growth and their response to varied light and CO2 concentration conditions and provide mechanistic support to estimate dynamic evapotranspiration and net ecosystem productivity at field-scale and a larger scale in paddy field ecosystems through the upscaling of leaf-level stomatal conductance, transpiration, and photosynthesis.


Introduction
Stomata play a crucial role in regulating water loss through transpiration and carbon dioxide (CO 2 ) uptake for photosynthesis, significantly influencing water use efficiency and plant productivity (Lawson and Vialet-Chabrand, 2019).Understanding the responses of stomatal conductance (g sw ), transpiration rate (T r ), and net photosynthetic rates (P n ) to environmental factors is essential to assess evapotranspiration and net ecosystem productivity in agroecosystems (Bellasio, 2023;Konieczna et al., 2023;Lv et al., 2024).Research into the intricate dynamics of g sw , T r , and P n across different environments improves predictive abilities and refines strategies for water utilization and agricultural optimization, which contributes to developing sustainable agricultural strategies aimed at maximizing productivity while minimizing water consumption (Elfadl and Luukkanen, 2006;Katul, 2023;Wu et al., 2023).
Several factors, including crop canopy structure (leaf area index, leaf tilt angle, etc.), leaf nutrient elements (nitrogen, chlorophyll, etc.), soil water-thermal conditions, and meteorological factors (solar radiation, CO 2 concentration, temperature, atmospheric humidity, etc.), have been widely studied for their influence on leaf g sw , T r , and P n (Chen et al., 2011;Xu et al., 2015;Liu et al., 2019).The impact of light and CO 2 , as the primary energy source and substrate for plant photosynthesis, on leaf g sw , T r , and P n have been extensively studied (Baroli et al., 2008, Li F, et al., 2023, Yi et al., 2023).With increased light intensity and CO 2 concentration, leaf P n initially increase rapidly and then slowly up to the maximum, followed by a declining trend or a stable state, which have been universally acknowledged on various crops (Kabir et al., 2023).Yu et al. (2004) reported that winter wheat g sw decreases with increased CO 2 concentration and increases with increased light intensity, Marıń et al. (2014) stated that tobacco T r is higher at high than at low light intensities, and Kirschbaum and McMillan (2018) showed that increasing atmospheric CO 2 concentrations reduce canopy transpiration.Additionally, the duration (such as cumulative time, thermal time accumulation, or radiant heat accumulation) after leaf emergence also leads to changes in leaf g sw , T r , and P n due to changes in both leaf traits (Legner et al., 2014;Scoffoni et al., 2016;Hirooka et al., 2018) and biomass sink-source relations (Kitajima et al., 2002;Xie and Luo, 2003) along with leaf aging from leaf appearance to senescence-for example, Vos and Oyarzun (1987) reported that potato P n and g sw decreased at nearsaturating irradiance with leaf age, Echer and Rosolem (2015) stated that cotton P n and g sw decreased in the order of 15-, 30-, 45-, and 60-day-old leaves.Locke and Ort (2014) showed that soybean P n decreased at a specific light intensity.However, the response of g sw , T r , and P n to light and CO 2 , respectively, are rarely reported for rice leaves with different durations after emergence.
As the most important staple food crop in the world, the threedimensional canopy structure of rice, describing the elongation process and spatial distribution of various organs (leaves, leaf sheaths, stems, and panicles), has been widely studied (Watanabe et al., 2005;Song et al., 2013).Temporal leaf evapotranspiration and photosynthesis with detailed 3D representation of canopy architecture are necessary to estimate seasonal variation in evapotranspiration and ecosystem productivity at field-scale and a larger scale in paddy field ecosystems, which are often achieved through the upscaling of leaf-level stomatal conductance, transpiration, or photosynthesis (Van der Zande et al., 2009;Chang et al., 2019;Shi et al., 2019).Measured light-saturated rice P n reaches a maximum at the fully developed stage and then declines gradually as leaves senesce (Wang et al., 2009) or decreases from the top (young leaves) to the base (old leaves) within the rice canopy (Murchie et al., 2002;Jin et al., 2004).The response of P n to light and CO 2 also changes as rice leaves age (Xu et al., 2019).Thus, it is well known that g sw and T r , under different light density and CO 2 concentration conditions, also vary among leaves with various durations after leaf emergence.However, the response of g sw and T r to light and CO 2 is rarely reported for rice leaves with different durations after leaf emergence.
The southern regions of the Yangtze River constitute the primary rice cultivation area in China (You et al., 2011).Understanding how the duration after leaf emergence affects P n , g sw , and T r under different light density and CO 2 concentration conditions is essential to unravel the physiological mechanisms of crop transpiration and photosynthesis and to assess seasonal changes in evapotranspiration and ecosystem productivity under different environmental conditions.Therefore, this study aimed to elucidate and analyze the influence of different days after leaf emergence (DAE) on P n , g sw , and T r as well as their quantitative relationships with DAE.This will help to understand the dynamic changes in P n , g sw , and T r and provide a reference to clarify the mechanism of transpiration and photosynthesis during the growth process of rice leaves.

Materials and methods
The Japonica Rice NJ46 was transplanted with 13 cm × 25 cm hill spacing on July 1, 2017 and harvested on October 26, 2017 in Kunshan, East China (31°15′50″ N, 120°57′43″ E) under field conditions.The rice field extended approximately 200 m in all directions.The region has a subtropical monsoon climate, with average temperature, mean relative humidity, and seasonal precipitation of 25.9°C, 76.9%, and 450.8 mm during the 2017 rice season.Irrigation, fertilizer, and pesticides were applied according to local farming practice (Guo et al., 2017;Li JP, et al., 2023;Lv et al., 2024).To record DAE for subsequent data collection, three latestemerged leaves on approximately 20 rice plants were tagged at 2-day intervals during tillering, jointing, and booting stages.Using a photosynthesis system (LI-6800; LI-COR, Lincoln, NE, USA) equipped with a red/blue LED light source (LI-6800-02B) and a charged CO 2 cartridge (CO 2 source), the response of leaf stomatal conductance (g sw ), transpiration rate (T r ), and net photosynthetic rate (P n ) to photosynthetically active radiation (PAR) and atmospheric CO 2 concentration (C a ) were measured for tagged leaves at various DAE values at booting and heading stages.The chamber temperature and relative humidity were set as 30°C and 70%, and the measurements were conducted under saturated soil moisture conditions at 8:00-12:00 a.m. on randomly selected sunny days during jointing and heading stages.For the response of g sw , T r , and P n to PAR, the C a and PAR were set at 400 mmol mol -1 (approximate atmospheric CO 2 concentration) and 2,000 mmol m -2 s -1 , and such a condition was maintained for 15 min for adaptation and stabilization of leaf photosynthesis prior to measurement.Then, leaf g sw , T r , and P n were recorded automatically at 120-s intervals at 19 PAR levels (in decreasing order of 2, 000, 1,950, 1,900, 1,800, 1,600, 1,400, 1,200, 1,000, 800, 600, 400, 300, 200, 150, 100, 70, 50, 30, and 0 mmol m -2 s -  1 ).For the response of g sw , T r , and P n to C a , the C a and PAR were set at 400 mmol mol -1 and 1,600 mmol m -2 s -1 [slightly lower than saturation light intensity (Xu et al., 2019) to prevent photo inhibition], and leaf g sw , T r , and P n were recorded automatically at 120-s intervals at 14 C a levels (in the order of 400,300,200,100,50,400,400,500,600,800, 1,000, 1,300, 1,500, and 1,800 mmol mol -1 ) after a 15-min pre-treatment.Totally, 37 response curves to PAR and 24 curves to C a were measured, evenly distributed across DAE values ranging from 3 to 55.

Light response of stomatal conductance, transpiration, and photosynthesis for rice leaves with different days after leaf emergence
The g sw , T r , and P n values were influenced by both the DAE and PAR (Figure 1).Under dark conditions (PAR = 0 mmol m -2 s -1 ), leaves at different DAE maintained relatively low g sw and T r and negative P n .As PAR increased, g sw , T r , and P n initially exhibited a linear and rapid increase, and then the increase rate (indicated by dg sw /dPAR, dT r /dPAR, and dP n /dPAR) gradually slowed down.When PAR reached a certain light intensity (referred to the saturation light intensity for g sw , T r , and P n , respectively), g sw , T r , and P n reached their maximum values.Subsequently, with further increases in PAR, there was a declining trend (for leaves at DAE lower than approximately 40 days) or a stable state (for leaves at DAE higher than approximately 40 days).The g sw , T r , and P n , as well as their increase rates with increasing PAR among leaves at different DAE, exhibited similar values under low PAR conditions and showed more pronounced differences as PAR increased.
In any PAR condition, leaf g sw linearly decreased with an increase in DAE, and the decrease rate (indicated by the absolute value of the slope of the linear regression line) increased with enhanced PAR (Figure 2).Under PAR of 0 and 100 mmol m -2 s -1 conditions, DAE had a negligible impact on leaf g sw , and the leaves consistently maintained a lower g sw value.Under PAR of 200, 400, and 800 mmol m -2 s -1 conditions, the slopes of g sw against DAE were -0.0018, -0.0038, and -0.0057, respectively; the leaf g sw significantly decreased with increasing DAE, and there are noticeable differences in both leaf g sw and the decrease rate among different PAR intensities.Under conditions of PAR higher than 1,200 mmol m -2 s -1 , the decrease rate in leaf g sw with DAE was approximately 0.007, and leaf g sw ranged from 0.127 to 0.659 mmol m -2 s -1 .Leaf g sw significantly decreased with increasing DAE, but the differences in both leaf g sw and the decrease rate were less pronounced among different PAR intensities.
Consistent with the variation in leaf g sw , leaf T r linearly decreased with an increase in DAE under any PAR condition, and the decrease rate increased with enhanced PAR (Figure 3).Under PAR conditions lower than 200 mmol m -2 s -1 , leaf T r external environmental demand for leaf evaporation is weak, and leaf T r remains consistently low, with no significant decrease in leaf T r with increasing DAE.Under PAR intensities of 400, 800, 1,200, 1,600, and 2,000 mmol m -2 s -1 , leaf T r respectively ranged from 1.015 to 4.265, 1.724 to 5.359, 1.938 to 7.790, 2.221 to 7.677, and 2.819 to 9.072 mmol m -2 s -1 , and the slopes of leaf T r against DAE, respectively, were -0.0325, -0.0464, -0.0666, -0.0771, and -0.0988.Under high PAR conditions (exceeding 400 mmol m -2 s -1 ), leaf T r significantly decreased, and the decrease rate becomes more pronounced with increasing PAR.Younger leaves can maintain higher T r under high light conditions to expedite transpirational cooling, enabling the leaves to remain within the optimal temperature range for physiological activities.As the leaves aged, physiological activity decreased, and leaf adaptability to light intensity decreased, resulting in lower T r under high light conditions.
Under no-light conditions (PAR = 0 mmol m -2 s -1 ), leaf P n was negative, and P n linearly increased with DAE (Figure 4).The leaves were unable to perform photosynthesis under zero light intensity, and leaves with low DAE exhibited a stronger metabolic activity, reflected in a higher respiration rate (manifested as negative values).Under a PAR of 100 mmol m -2 s -1 , leaf P n remained at approximately 3.6 mmol m -2 s -1 , with no significant change in leaf P n with increasing DAE.Under PAR conditions higher than 200 mmol m -2 s -1 , leaf P n significantly decreased with increasing DAE, and the magnitude of decrease became more pronounced with enhanced PAR.

CO 2 response of stomatal conductance, transpiration and photosynthesis for rice leaves with different days after emergence
The C a considerably influenced g sw , T r , and P n in rice leaves (Figure 5).The diffusion of CO 2 from the outside to the inside of the leaf primarily relied on stomata; an increase in C a led to a reduction in leaf g sw , followed by a decrease in leaf T r (Figures 5A, B).Leaf g sw and T r gradually decreased with increasing C a and DAE, and their decreasing rate slowed down as C a increased.When C a increased to approximately 1,500 mmol mol -1 , leaf g sw and T r stabilized at the minimum values.Under the C a range of 0 to 1,800 mmol mol -1 , leaf g sw respectively ranged from 0.103 to 0.693, 0.171 to 0.411, 0.139 to 0.458, 0.133 to 0.404, 0.135 to 0.247, and 0.104 to 0.165 mol m -2 s -1 , and leaf T r respectively ranged from 1.426 to 7.895, 2.694 to 5.622, 2.431 to 6.401, 2.423 to 5.912, 2.326 to 3.872, and 1.615 to 2.514 mmol m -2 s -1 for DAE of 1-10, 11-20, 21-30, 31-40, 41-50, and 51-60 days.Both leaf g sw and T r decreased with increasing DAE under specific C a conditions.Leaves at smaller DAE maintained higher g sw and T r at low C a , indicating that vigorously growing leaves sustained higher g sw for physiological processes (such as transpiration and photosynthesis) and exhibited robust physiological activity even under low C a conditions.There was a relatively small difference in leaf g sw and T r among leaves at different DAE at high C a concentrations.Leaves with larger DAE (41-50 and 51-60 days) showed limited sensitivity of g sw and T r to changes in C a concentration, maintaining consistently lower values regardless of the variations in C a concentration.(A-C) The light response of stomatal conductance, transpiration rate, and net photosynthetic rate for rice leaves with different ranges of days after leaf emergence ("m~n d" in the legend indicates the days after leaf emergence; ranges from m to n).
The leaf P n at different DAE exhibited a similar trend with changing atmospheric C a (Figure 5C).The increase rate of leaf P n (indicated by dP n /dC a ) gradually slowed down with increasing DAE.As C a increased, rice leaf P n initially increased rapidly in a linear fashion, and the increase rate subsequently decreased, and leaf P n gradually reached its maximum value, resulting in either a stable or a declining P n .Under CO 2 concentrations lower than 50 mmol mol -1 , leaf photosynthesis was constrained by the available CO 2 concentration; larger stomatal conductance could not compensate for the impact of low CO 2 concentration, resulting in lower leaf photosynthesis than respiration, leading to CO 2 emission (negative P n values).Within the C a range of 0 to 1,800 mmol mol -1 , leaf P n ranged from -0.437 to 41.866, -0.419 to 39.614, -0.491 to 40.345, -0.639 to 29.344, -0.485 to 19.135, and -0.504 to 10.657 mmol m -2 s -1 for DAE of 1-10, 11-20, 21-30, 31-40, 41-50, and  (A-H) Impact of days after leaf emergence on stomatal conductance under different photosynthetically active radiation conditions.The relationships between g sw , T r , and P n and DAE could be fitted using quadratic regression equations (Figures 6-8).Under C a of 50, 200, 400, 600, 1,000, and 1,800 mmol mol -1 , leaf g sw respectively ranged from 0.132 to 0.535, 0.122 to 0.474, 0.134 to 0.478, 0.129 to 0.390, 0.111 to 0.316, and 0.046 to 0.224 mmol m -2 s -1 .Leaf g sw decreased along with increasing C a .As DAE increased, leaf g sw initially remained at higher values and subsequently Leaf T r exhibited a similar trend to leaf g sw (Figure 7).Under C a of 50, 200, 400, and 600 mmol mol -1 , leaf T r for different DAE respectively ranged from 1.876 to 7.007, 1.743 to 7.810, 1.905 to 6.467, and 1.815 to 6.202 mmol m -2 s -1 .Leaf T r decreased with increasing C a , and rice leaves at small DAE maintained a higher T r at low C a .As DAE increased, leaf T r initially remained at higher values and then gradually decreased.At C a of 1,000 and 1,800 mmol mol -1 , the impact of DAE on T r diminished, and high CO 2 concentration inhibited stomatal aperture and transpiration.
(A-H) Impact of days after leaf emergence on net photosynthetic rate under different photosynthetically active radiation conditions.Lv et al. 10.3389/fpls.2024.1397948Frontiers in Plant Science frontiersin.org The variation in leaf P n with DAE under different C a is depicted in Figure 8.At C a of 50 mmol mol -1 , the leaf P n at different DAE consistently remained at approximately -0.5 mmol m -1 s -1 .This is primarily attributed to the limitation of photosynthetic capacity by low CO 2 concentrations, where leaf respiration exceeded photosynthesis, resulting in CO 2 release.At C a of 200, 400, 600, 1,000, and 1,800 mmol mol -1 , leaf P n respectively ranged from 1.690 to 13.114, 5.484 to 27.375, 6.694 to 41.858, 8.576 to 47.116, and 9.304 to 47.137.Leaf P n rapidly increased with rising C a , reaching its peak at approximately 1,000 mmol mol -1 C a , with no considerable difference between 1,000 and 1,800 mmol mol -1 C a .When C a exceeded 200 mmol mol -1 , leaf P n remained relatively high at smaller DAE and gradually decreased with further increases in DAE.This indicated that vigorously growing leaves exhibited higher P n , and leaf photosynthetic capacity decreased as leaves age, leading to a decline in carbon assimilation.(A-C) CO 2 response of stomatal conductance, transpiration rate, and net photosynthetic rate of rice leaves with different ranges of days after leaf emergence ("m~n d" in the legend indicates the days after leaf emergence; ranges from m to n).Lv et al. 10.3389/fpls.2024.1397948 in Plant Science frontiersin.org4 Discussion

Effect of days after leaf emergence on the light response
As PAR was enhanced, leaf g sw , T r , and P n initially exhibited a linear and rapid increase, followed by a gradual slowdown in the increase rate, eventually reaching a maximum value and then stabilizing or slightly decreasing thereafter (Figure 1).Similar trends have been observed in the flag leaves of winter wheat (Inoue et al., 2004;Carmo-Silva et al., 2017).Under no-light conditions (PAR = 0 mmol m -2 s -1 ), the leaves were unable to undergo photosynthesis, resulting in metabolic CO 2 emission (with leaf P n showing as a negative value).Leaves at smaller DAE released more CO 2 due to their vigorous metabolic activity (Pantin et al., 2012).Under low-light conditions, limited atmospheric evaporative capacity and insufficient PAR for photosynthesis led to lower g sw , T r , and P n regardless of the variations in DAE.As PAR intensified, leaf stomatal opening widened, leading to an increase in g sw .Larger stomatal apertures allowed a greater influx of CO 2 (providing an ample supply for leaf photosynthesis) and output of water vapor through the stomata; thus, leaf P n and T r increased.Simultaneously, the increased atmospheric evaporative capacity caused by enhanced PAR also resulted in higher T r .Leaves with larger DAE reached the light saturation point earlier, and g sw , T r , and P n , under saturated light conditions, decreased with increasing DAE, suggesting that young leaves could maintain larger stomatal apertures for efficient transpiration and photosynthesis under high light intensity (high T r and P n ).As the leaves aged, their adaptation to high light weakened, and leaves with larger DAE could not fully utilize high light intensity for photosynthesis.
Under a specific PAR condition, g sw , T r , and P n showed a consistent linear decrement with the increase in DAE (Figures 2-4).This finding was congruent with the decline in g sw and P n with potato leaf senesced (Vos and Oyarzun, 1987).Echer and Rosolem (2015) also asserted that cotton leaf DAE had nominal impact on leaf P n under low PAR, while P n was notably higher in 15-and 30-day-old (A-F) Impact of days after leaf emergence on stomatal conductance under different atmospheric CO 2 concentration conditions.Lv et al. 10.3389/fpls.2024.1397948Frontiers in Plant Science frontiersin.orgleaves compared to 45-and 60-day-old leaves when PAR exceeded a threshold, with both T r and g sw reduced as the leaves aged and the light intensity waned.Hossain et al. (2007) and Jin et al. (2004) reported that rice g sw , T r , and P n , at particular PAR, decreased significantly with lowering leaf position, which was consistent with the current research, as newly emerged rice leaves appeared in the upper canopy, implicating a reduction in leaf DAE as leaf position decreased.Generally, rice leaf photosynthesis was highly related to leaf nitrogen level, efficiencies of radiant energy utilization, electron transport, and photophosphorylation, and these values decreased with leaf aging (or downward leaves) (Murchie et al., 2002;Suzuki et al., 2009;Okami et al., 2016;Yang et al., 2016), which also agreed with the decreased P n .In contrast, Wang et al. (2009) reported that the measured light-saturated rice g sw , T r , and P n reached the maximum at the last second fully developed leaf and then declined gradually in downward leaves at nine-leaf age (an indicator representing the developmental progress of plants) stage (tillering stage correspondingly).Xu et al. (2019) also stated that light-saturated rice P n peaked at around 10 days after leaf emergence and then decreased as leaves aged.The discrepancy with the current study might be attributed to low-frequency measurement for photosynthetic characteristics under smaller DAE, as the measurement was inconvenient due to the small leaf area before they were fully expanded.Additionally, the measurement in the current study began at DAE of 3 days, at which time the leaves had a large leaf area.Consequently, the study did not monitor the increase in leaf g sw , T r , and P n during the leaf expansion process.

Effect of days after leaf emergence on the CO 2 response
As C a increased, leaf g sw and T r gradually decreased, while P n increased linearly and rapidly, and the amplitude of variations in g sw , T r , and P n decelerated, eventually leading to a stabilization of minimal g sw and T r and an elevation of P n to its peak, subsequently maintaining (A-F) Impact of days after leaf emergence on transpiration rate under different atmospheric CO 2 concentration conditions.Lv et al. 10.3389/fpls.2024.1397948Frontiers in Plant Science frontiersin.orgstability or experiencing a slight decline (Figure 5).Yasutake et al. (2016) found that 1,000 mmol mol -1 C a significantly increased sweet pepper P n but decreased g sw and T r compared with 400 C a .Ahmed et al. (2022) reported that P n increased and g sw and T r decreased in the order of 500, 1,000, and 1,500 mmol mol -1 C a .This was consistent with the decreased g sw and T r and increased P n with leaf aging observed in the current study.Inamoto et al. (2022) showed that the increase in Oriental Hybrid Lily P n was greater in the low C a range (380 to 1,000 mmol mol -1 ) and lower in the high C a range (1,000 to 2,000 mmol mol -1 ), which agreed with the amplitude of variations in P n .
Under specific C a , the leaf g sw , T r , and P n remained at a relatively high level when DAE was less than approximately 25 days and then gradually decreased with the further increase in DAE (Figures 6,7,8).Chlorophyll activity, Rubisco activity, RuBP regeneration capacity, and nitrogen content (positively correlated with the photosynthetic potential of leaves) generally exhibited an increasing trend during the leaf expansion phase, followed by the maintenance of relatively high values, and then decreased as the leaves aged (Murchie et al., 2002;Suzuki et al., 2009;Gunasekera et al., 2013), which might be the primary reasons for the variation in g sw , T r , and P n .At lower C a concentrations, leaves at a smaller DAE maintained higher g sw to facilitate atmospheric CO 2 entering for transpiration and photosynthesis.Leaves at a greater DAE had weaker adaptability to external environments, maintaining lower levels of g sw , T r , and P n regardless of C a level.When C a exceeded a certain level, C a exerted a suppressive effect on stomatal conductance to reduce transpiration, but the photosynthetic rate did not decrease.

Conclusions
This study investigated the dynamics of stomatal conductance g sw , transpiration rate T r , and net photosynthetic rate P n in rice leaves across (A-F) Impact of days after leaf emergence on net photosynthetic rate under different atmospheric CO 2 concentration conditions.Lv et al. 10.3389/fpls.2024.1397948Frontiers in Plant Science frontiersin.orgvarying light intensities and CO 2 conditions during leaf development.
The key conclusions drawn from the findings are as follows: (1) Response to photosynthetically active radiation PAR: Increasing PAR led to an initial rapid and linear increase in g sw , T r , and P n , followed by a more gradual rise to maximum values, with subsequent stabilization or decline.Notably, old leaves reached their maximum g sw , T r , and P n earlier and at smaller magnitudes compared to young leaves.Additionally, a linear decreasing trend in g sw , T r , and P n with increasing DAE was observed, with the decrease rate slowing down with reduced PAR.
(2) Response to atmospheric CO 2 concentrations C a : With increasing C a , g sw and T r decreased gradually to a stable minimum value, while P n a linear and slow increase up to a maximum before stabilizing or decreasing.Under specific C a conditions, rice leaf g sw , T r , and P n initially remain at higher values and then gradually decrease with increasing DAE.
These conclusions provided crucial mechanistic insights to estimate dynamic evapotranspiration and net ecosystem productivity at both field-scale and larger scales in paddy field ecosystems by upscaling leaf-level physiological processes.This knowledge can inform more accurate predictions and management strategies to optimize agricultural practices and enhance the sustainability of rice cultivation amidst changing environmental conditions.
2 concentrations (especially at a C a of 1,800 mmol mol -1 ) inhibited stomatal aperture, and the leaf g sw at different DAE consistently remained at lower values.